Reviews of Plasma Physics / Voprosy Teorii Plazmy / Вопросы by A. I. Morozov, L. S. Solov’ev (auth.), Acad. M. A.

By A. I. Morozov, L. S. Solov’ev (auth.), Acad. M. A. Leontovich (eds.)

In the curiosity of velocity and economic system the notation of the orig­ inal textual content has been retained in order that the move made from vectors A and B is denoted via [AB], the dot product via (AB), the Laplacian operator via ~. and so on. it may even be worthy mentioning that the temperature is usually expressed in strength devices within the Soviet literature in order that the Boltzmann consistent should be lacking in a variety of generic expressions. In concerns of terminology, every time pos­ sible a number of kinds are used while a time period is first brought, e. g. , magnetoacoustic and magnetosonic waves, "probkotron" and reflect laptop, and so forth. it truly is was hoping during this option to support the reader to narrate the phrases used right here with these in present translations and with the traditional nomenclature. generally the procedure of literature quotation utilized in the bibliographies follows that of the yankee Institute of Physics "Soviet Physics" sequence. aside from the cor­ rection of a few noticeable misprints the textual content is that of the unique. we want to convey our gratitude to Academician Leontovich for kindly delivering the most recent corrections and additions to the Russian textual content. v CONTENTS Steady-State Plasma stream in a Magnetic box A. I. Morozov and L. S. Solov'ev advent. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 bankruptcy 1. Acceleration Mechanisms , • • • • • • • • • • . 2 §1. Microscopic photograph of Plasma Acceleration . . . . . . . . . . . . . . . . . . . 2 §2.

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111) The geometry of the outer electrode will depend on whether the compression occurs with a velocity v- 0, a nonvanishing constant velocity, or an increasing velocity. The lines of the electric current are governed by the equation Hr § 5. = const. 112) Flow Velocity Equal to Signal Velocity at Some Point We now treat the case in which the flow velocity reaches the signal velocity at some point. It turns out that the critical surface, at which v =v 5 , has certain distinctive features. In particular, if there exists a planar cross section of the channel z = z * = const in which the velocity has only the single component v z, then the critical velocity, which is equal to the signal-propagation velocity, is reached in this cross section [20].

Const. 112) Flow Velocity Equal to Signal Velocity at Some Point We now treat the case in which the flow velocity reaches the signal velocity at some point. It turns out that the critical surface, at which v =v 5 , has certain distinctive features. In particular, if there exists a planar cross section of the channel z = z * = const in which the velocity has only the single component v z, then the critical velocity, which is equal to the signal-propagation velocity, is reached in this cross section [20].

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